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1 erials to investigate light-assisted battery charging.
2 lizing the reactive bromine generated during charging.
3 x reactions in layered oxides during initial charging.
4 uration corresponding to lithium ion battery charging.
5 chromatography (LC), due to analyte multiple charging.
6  the external dimensions of the anode during charging.
7 be minimized by limiting the voltage used on charging.
8  that reside in the bulk of the liquid after charging.
9 n release is then kinetically favored during charging.
10 % more and ~20% fewer emissions than daytime charging.
11 ates from the continuous oxygen release upon charging.
12 clopentane, and cyclohexane) to improve tRNA charging.
13  as well as revenue losses due to time spent charging.
14  owing to dielectric breakdown(14), electric charging(15) and biofouling(16).
15 nput voltage of stack SMFCs up to 5.02 V for charging a cell phone battery.
16 lighting up a warning indicator, sustainably charging a commercial capacitor, and powering a smart wa
17 that oxygen is extracted from the lattice on charging a Li1.2[Ni0.13(2+)Co0.13(3+)Mn0.54(4+)]O2 catho
18                                         Yet, charging a price to screen out nonusers may screen out p
19 system, which provides enough d.c. power for charging a smart watch or phone battery, is also success
20 included patients who did not have access to charging a smartphone.
21                                       During charging, a uniform Mg film was deposited on the electro
22                               Potentiostatic charging abuse tests of Li-metal pouch cells result in d
23                             It is shown that charging almost always involves ion exchange (swapping o
24 -tRNA synthetases (ARSs) are responsible for charging amino acids to cognate tRNA molecules, which is
25 phasial chemistry occurs (during the initial charging), an electric double layer forms at the electro
26                        In London, congestion-charging and a citywide low-emission zone failed to brin
27 t that neutral osmolytes may have on surface charging and Coulomb interactions.
28 en faster, while also reducing both electron charging and damage to the samples.
29 ve the net effect of reducing the capacitive charging and decreasing the time required to achieve ste
30  which can support high energy density, fast charging and discharging capability, cycle stability, sa
31 h greater pyrolysis temperature due to lower charging and discharging capacities, although the chargi
32 ctrons more than three times faster than the charging and discharging cycles of surface functional gr
33 bserved sub-microsecond, continuous membrane charging and discharging dynamics.
34 ts BPC is a phenomenon balanced by localized charging and discharging events across the membrane.
35 the electrolyte and its functionality during charging and discharging is intricate and involves multi
36 ing and discharging capacities, although the charging and discharging kinetics remain unchanged.
37                                   During the charging and discharging of lithium-ion-battery cathodes
38 c synthesis and characterization, show rapid charging and discharging of NP within 100 fs, with assoc
39  open up opportunities to greatly accelerate charging and discharging of subnanometre pores without c
40 dergonic overall, is facilitated by temporal charging and discharging of the molecule placed in the n
41 rdered LNMO as a cathode material during the charging and discharging process.
42 e contradictory requirements of accelerating charging and discharging processes, we select two pseudo
43 ing and leaving such pores, which slows down charging and discharging processes.
44 , by electrochemically switching between the charging and discharging status of battery electrodes th
45                                          The charging and discharging times of the super capacitors h
46 more energy, without compromising their fast charging and discharging times.
47              By analyzing the kinetics of Ub charging and discharging, we identified proximal active
48 te growth and infinite volume changes during charging and discharging, which lead to short lifespan a
49  operation of an internal supercapacitor for charging and discharging.
50 tween marginal emission rates during battery charging and discharging.
51 aterials undergo large volume changes during charging and discharging.
52 rn the phase transformations associated with charging and discharging.
53                                         Fast-charging and high-energy-density batteries pose signific
54 ping reviews were conducted for anticipatory charging and monitoring of physiological parameters duri
55 te amino acid selection, transfer RNA (tRNA) charging and mRNA decoding on the ribosome.
56                  Use of renewable energy for charging and operation, ease of component recycling/reus
57 ng microscope, thus allowing gate-controlled charging and spectroscopic interrogation of individual t
58 or glutaminase inhibitors restores tRNA(Gln) charging and the levels of polyglutamine-containing prot
59 ate complex to be stored after photochemical charging and used as a reagent in dark reactions, such a
60 onductivity transition, quantized capacitive charging, and anisotropic conductivity characteristics.
61 tography (LC) solvents improves sensitivity, charging, and chromatographic resolution for acidic and
62      What mechanism(s) can explain such high charging, and what is the ultimate limit?
63 t(4,5) Li(3+x)V(2)O(5) can be used as a fast-charging anode that can reversibly cycle two lithium ion
64 magnetically enhanced photon-transport-based charging approach, which enables the dynamic tuning of t
65 lower phase), an aqueous solution of K2MCl4 (charging arm; M = Pt, Pd), and an aqueous solution of ex
66 widely applicable for investigations of tRNA charging as a parameter in biological regulation.
67 henotypes, and further support impaired tRNA charging as the primary mechanism of recessive ARS-relat
68 U4 to be a bona fide E2 enzyme through an E2 charging assay.
69 ion model, we estimated GHG emissions for EV charging at two EV penetration rates, 5% and 30%, and fi
70 thermoelectric devices to high-capacity fast-charging batteries and integrated high-speed electronic
71                                         Fast-charging batteries typically use electrodes capable of a
72                                       A fast-charging battery that supplies maximum energy is a key e
73                        This unique selective charging behavior in different confined porous structure
74 low fleet operators to manage their drivers' charging behavior, along with collection and integration
75 f these proteins is key to realizing a 'self-charging biophotonic device' that not only harvests ligh
76   We present a transparent and flexible self-charging biosupercapacitor based on an optimised mediato
77        A UbV targeting Ube2D1 did not affect charging but greatly attenuated chain elongation.
78 , night charging nearly matches low emission charging, but night charging emissions increase with 30%
79 pplied, going beyond the traditional view of charging by counter-ion adsorption.
80 ults reveal that the stoichiometry-dependent charging by the support can be used to tune the selectiv
81 on regimes, which shows that the target self-charging can be optimised at a pulse duration of few hun
82 xidation reveals that the complex retained a charging capacity of 72% after four cycles.
83              Here we report a direct thermal charging cell, using asymmetric electrodes of a graphene
84                               Direct thermal charging cells attain a temperature coefficient of 5.0 m
85 he measured reactivity trends correlate with charging characteristics of a Pt13 cluster on the SiO2 f
86 tery operation, including both slow and fast charging conditions.
87  Li metal deposition process under different charging conditions.
88              The electricity grid-based fast-charging configuration was compared to lithium-ion SLB-b
89 ikelihood of lithium metal plating if proper charging controls are used, alleviating a major safety c
90 n charging infrastructure, while intelligent charging coordination can greatly reduce requirements fo
91  electron transfer kinetics, high background charging current and low current density arising from po
92                                          The charging current associated with the nanosecond screenin
93  4th to 12th harmonics after quantifying the charging current data using the time-domain response.
94 On the one hand, time dependent decay of the charging current mitigates its impact on the current con
95                 Analysis of the decay in the charging current suggests that the desired screening may
96                      The potential-dependent charging current upon the formation of the microscopic e
97 lly and experimentally the effect of induced charging currents on the fast-scan cyclic voltammetry.
98              Due to the existence of induced charging currents, the capacitive contribution to the to
99 erimental comparisons show that the designed charging cycle can enhance the charging rate, improve th
100                 Here, we rationally design a charging cycle to maximize energy-storage efficiency by
101 shown to extend the battery lifetime between charging cycles while powering a load.
102  excellent mechanical robustness, high photo-charging cycling stability (98.7% capacitance retention
103 esting a need for policy that can smooth out charging demand after midnight.
104 where non-reversible features during in situ charging-discharging cycles were observed.
105 ifold advantages of high power density, fast charging-discharging, and long cyclic stability.
106 red in the time domain from constant-current charging/discharging and cyclic voltammetry tests, and f
107 ng the POMs from chemical degradation during charging/discharging and facilitating efficient electron
108                             Through hydrogen charging/discharging by applying voltages of only ~1 V,
109 rial that shows high specific capacity, fast charging/discharging capability, and long cycle life for
110                                 After 17h of charging/discharging cycles a remarkable current enhance
111 in energy-dense lithium metal batteries, the charging/discharging process results in structural heter
112  applied, and shows no hysteresis during the charging/discharging processes.
113 ctric capacitors, although presenting faster charging/discharging rates and better stability compared
114  and 100 uL), bending radii (10, 15, 20 mm), charging/discharging stability (4000 cycles), and washab
115 alytical calculations of capacitive membrane charging/discharging, also known as accelerated membrane
116 Li x Sn --> Sn --> SnO2 /SnO2-x cycle during charging/discharging.
117 rejection, i.e., during doping/de-doping and charging/discharging.
118 lmost all oxygen-redox compounds, is lost on charging, driven in part by formation of molecular O(2)
119 id data from 2018 and 2019 (alongside hourly charging, driving, and temperature data) to estimate EV
120 vided, in addition, new evidence of electric charging during the vapor plume cloud processes.
121 ing, surface reconstructions, contamination, charging effects and surface roughness in single-particl
122 ere offer a convenient approach to probe the charging effects in perovskite solar cells.
123 ng the reversibility of the photoresponse to charging effects.
124 tricity grid and therefore the cost for fast-charging electric vehicles (EVs).
125 rly matches low emission charging, but night charging emissions increase with 30% EV penetration, sug
126 ice lowers parasitic capacitance, increasing charging energy EC.
127 modifications independently confer high tRNA charging fidelity to the otherwise promiscuous, unmodifi
128 ergoes a temperature dependent shift in tRNA charging fidelity, allowing the enzyme to conditionally
129 trands to prevent sufficient downstream cell charging for AP propagation.
130 is work highlights the importance of surface charging for electrochemical kinetics and mass transport
131 for hindering Auger decay with postsynthetic charging for suppressing parasitic ground-state absorpti
132                                              Charging fraction is obtained by counting the fraction o
133                                         tRNA charging fractions can be measured for individual tRNA s
134                  By monitoring the capacitor charging frequencies, which are influenced by the concen
135 characterization of the power generation and charging frequency characteristics in glucose analyte ar
136 hium ions required for more power and faster charging generates significant stresses and strains in t
137                        It can also enable EV charging in areas where grid limitations would otherwise
138  packs to perform engine cold cranking, slow charging in cold weather, restricted regenerative brakin
139 plementation assays, and assessments of tRNA charging indicate that each CARS variant causes a loss-o
140 nerally uniform throughout the particle, the charging induces a strong depth dependency in transition
141 et applications has been hindered by lack of charging infrastructure and long charging times.
142          To address both the need for a fast-charging infrastructure as well as management of end-of-
143 scuss several options for nudging, including charging infrastructure availability, battery design, an
144 l policy tweaks, oil price, battery cost and charging infrastructure for the Chinese passenger vehicl
145 cle trajectories and energy consumption, (2) charging infrastructure installation costs, and (3) real
146 p-down policy targets can spur investment in charging infrastructure, while intelligent charging coor
147 e V(5+) and S(2-) containing intermediate on charging instead of VS(4).
148                                  A diffusion charging instrument (DiSCMini), that simulates alveolar
149      Herein, we demonstrate a flexible solar-charging integrated unit based on the design of printed
150 sed from understanding whether impaired tRNA charging is a critical component of this disease to eluc
151                                         More charging is obtained with the smaller tip sizes for prot
152 t to an operating LiMn(2)O(4) cathode during charging leads to a remarkable lowering of the battery c
153 cally with methionine engendered at the tRNA charging level occurs in mammalian cells, yeast and arch
154                                    These low charging levels were validated using acid denaturing gel
155 CN4 response, despite maintenance of tRNAGln charging levels, revealing that normally, the aaRS popul
156  than does a battery using a commercial fast-charging lithium titanate anode or other intercalation a
157 lectrostatic doping is not the only route to charging localized quantum emitters and another path for
158 o identify other metal oxide anodes for fast-charging, long-life lithium-ion batteries.
159 t as electron source greatly exceeds the net charging measured in a Faraday pail/electrometer set up,
160 m the distinct step-by-step photon-transport charging mechanism and the increased latent heat storage
161                               We introduce a charging mechanism parameter that quantifies the mechani
162 mputer simulations have shown that different charging mechanisms can then operate when a potential is
163 al studies to give a detailed picture of the charging mechanisms of supercapacitors.
164       Increased understanding and control of charging mechanisms should lead to new strategies for de
165 lain the factors that control supercapacitor charging mechanisms, and to establish the links between
166 ed analyte ions despite presumably different charging mechanisms.
167 alculated as increased system emissions from charging minus avoided emissions from discharging.
168 nstant current (CC) or constant voltage (CV) charging mode with pH ranged from 5 to 9 in the feed sol
169  acquired results and an analytical membrane-charging model validates the utility of this technique.
170 ed droplets enable the generation of 2D self-charging nanostructured networks on a large scale.
171                     At 5% penetration, night charging nearly matches low emission charging, but night
172                  It is proposed that surface charging occurs through the adsorption of the imidazoliu
173 rtant skills including reactor construction, charging of a back-pressure regulator, assembly of stain
174                                          The charging of a mesoscopic TiO2 layer in a metal halide pe
175 e been investigated, but rapid electrostatic charging of all such devices has hindered these efforts.
176             We investigate the electrostatic charging of an agitated bed of identical grains using si
177                   The latter is triggered by charging of Asp164, the first proton carrier.
178 ies are observed, and the extent of multiple charging of corresponding ions indicates a partial loss
179 hanges in dissipation due to single-electron charging of individual quantum dots in carbon nanotubes.
180 E2 variant Ube2V1 did not interfere with the charging of its partner E2 enzyme but inhibited formatio
181 hat can strongly exceed the gas temperature; charging of nanoparticles through plasma electrons reduc
182                                          The charging of protein ions formed by nanoelectrospray ioni
183 technique, which exploits the transient self-charging of solid targets irradiated by intense laser pu
184  of implantable medical devices and wireless charging of stationary electric vehicles.
185  about 1 nm with simultaneous imaging of the charging of the DNA molecules that is of the order of le
186 tion for removal of the large current due to charging of the electrical double layer as well as surfa
187                                   Capacitive charging of the electrical double layer at opposing ends
188  transglutaminase cross-linking and niosomes charging of the protein solution enhanced the gelation p
189                                              Charging of the well-dissolved alkaline starch suspensio
190          In contrast, all other tRNAs retain charging of their cognate amino acids in a manner that i
191 reaction in protein biosynthesis, namely the charging of transfer RNAs (tRNAs) with their cognate ami
192 n and reduced total translation, the reduced charging of tRNA(Gln) in amino-acid-deprived cells also
193 TD to include genes implicated in amino acid charging of tRNA, which is required for the last step in
194 e type of charge injection, i.e., capacitive charging or ion intercalation, via the choice of the cha
195 nd tunable phase shift without electrostatic charging or unwanted electron scattering.
196 cribes an effective fundamental strategy for charging organic liquids, including nonpolar organic liq
197 iently use solar energy to overcome the high charging overpotential of conventional zinc-air batterie
198                       The emission impact of charging pattern varies by region.
199 of the reduction depends significantly on EV charging patterns and hourly power grid variations.
200  are found to be key factors determining the charging performance of sunlight-promoted zinc-air batte
201 e hybridized nanogenerator has a much better charging performance.
202 n was continuous (i.e., it did not require a charging period and did not vary during each step of a c
203 ery different areal capacities over the same charging period.
204                    The understanding of this charging phenomenon and of the related intense fields, w
205 ss-of-function alleles, suggesting that tRNA charging plays a central role in disease pathogenesis.
206  growth of renewable electricity generation, charging plug-in hybrid electric vehicles (PHEVs) from t
207 ytic acid-doped polyaniline as a novel redox-charging polymer support enabling the reagentless assayi
208  zinc-air battery with significantly reduced charging potential below the theoretical cell voltage of
209  number of ions in the absence of an applied charging potential.
210 onophobic pores in the absence of an applied charging potential.
211  method for quantifying the Fermi levels and charging potentials of free-standing colloidal n-type Zn
212                    A novel and scalable self-charging power textile is realized by combining yarn sup
213 gy in lipidomics, the potential for multiple charging presents unique challenges for CL identificatio
214                       Therefore, the arduous charging procedure of the reaction autoclave in a gloveb
215 dered to have significant influence over the charging process and therefore the overall performance o
216               Here, the CE and triboelectric charging process are studied for a metal-dielectric case
217 r propose that it is possible to control the charging process resulting in comprehensive enhancements
218 ter and sodium-ion during the high potential charging process results in the shrinkage of interlayer
219 on in time, giving a useful insight into the charging process, generation and distribution of fields.
220 a key step of water decomposition during the charging process, which broadens the voltage window of a
221  considerably lower overpotential during the charging process.
222  two-phase coexistence throughout the entire charging process.
223 nia and New York, respectively, overnight EV charging produces ~70% more and ~20% fewer emissions tha
224 ay governs the morphology of the discharging/charging products in Li-O2 cells.
225 eriments were undertaken to examine the self-charging properties of the material and to develop an un
226  functions of many of these upregulated tRNA charging proteins may together promote WS disease pathog
227 odology, we rapidly identify high-cycle-life charging protocols among 224 candidates in 16 days (comp
228 oltage profiles of six-step, ten-minute fast-charging protocols for maximizing battery cycle life, wh
229  to efficiently probe the parameter space of charging protocols.
230                                           On charging, quantitative LiOH oxidation occurs at 3.1 V, w
231 detachment is positively correlated with the charging rate and that smaller particles exhibit a highe
232 , the optical charging strategy improves the charging rate by more than 270% and triples the amount o
233                        Here we show that the charging rate of a cathode can be dramatically increased
234 port across the silicon particles limits the charging rate of batteries.
235   A serious limitation, however, is the slow charging rate used to obtain the full capacity.
236                                       A high charging rate usually leads to sacrifices in capacity an
237 hows highly stable battery cycling at a fast-charging rate with a high energy density beyond those of
238 far, there have been no ways to increase the charging rate without losses in energy density and elect
239  the designed charging cycle can enhance the charging rate, improve the maximum energy-storage effici
240 llers to improve the thermal-diffusion-based charging rate, which often leads to limited enhancement
241 mance of pseudocapacitive electrodes at fast charging rates are typically limited by the slow kinetic
242 ge materials, to simultaneously achieve fast charging rates, large phase-change enthalpy, and high so
243 ically necessary dislocations provide deeper charging reactions, indicating that dislocations may fac
244 Directly harvesting solar energy for battery charging represents an ultimate solution toward low-cost
245 ntown vs suburb, and an optimal low emission charging scenario, matching charging time with the lowes
246 erson-level travel activity data to simulate charging scenarios.
247 o EV penetration rates, 5% and 30%, and five charging scenarios: home, work and shopping, night, down
248 om the mean CO2 emissions factor for a given charging site among both marginal and average emissions
249 s might be utilised as part of a future self-charging solar device.
250 nce these organic batteries are excelling in charging speed and cycling stability.
251  which often leads to limited enhancement of charging speed and sacrificed energy storage capacity.
252           This binding is independent of the charging state of tRNA but is regulated by the redox sta
253  of components, their conformation and their charging state.
254 ucture installation costs, and (3) real-time charging station availability.
255 ic-vehicle charging using 10 methods at nine charging station locations around the United States.
256  analysis presented here directly couple the charging status of bound biomolecules to readout of liqu
257  achieving identical desalination during the charging step.
258 h conventional thermal charging, the optical charging strategy improves the charging rate by more tha
259 based energy storage is proposed for EV fast-charging systems.
260                                         The 'charging' (that is, ENSO imprinting the North Tropical A
261                                     However, charging the cross-linked protein solution with niosomal
262 fficient than its cytoplasmic counterpart in charging the mitochondrial tRNA(Gly) isoacceptor, which
263                                         Upon charging the molecule in a gated junction, we found repr
264                                             "Charging" the second type of particles with NO was reali
265 g acoustic streaming electrolyte flow during charging, the device enables dense Li plating and avoids
266           Compared with conventional thermal charging, the optical charging strategy improves the cha
267                                       During charging, the oxidation reaction at significantly reduce
268 ectroscopy analysis suggest that during deep charging, the precoated Se will initially substitute som
269 h has focused on factors such as nanocrystal charging, the ratio of ligand length to core radius, cor
270 size-dependent interplay of the metal domain charging, the relative band-alignments, and the resultin
271 O3 (-) indicates that LiOH can be removed on charging; the electrodes do not clog, even after multipl
272 epletion gradients in the electrolyte during charging, they rapidly develop porosity, dendrites, and
273 al patterns of electricity generation and EV charging, this study operationalizes the concept of marg
274  detectable signal varies in relation to the charging time and resistive and capacitive noise.
275 eads to a remarkable lowering of the battery charging time by a factor of two or more.
276 relatively weakly coupled systems within the charging time constant.
277 ms, the scan rate corresponding to nanoscale charging time constants appears to be suitable for the u
278      In the setting of diminished Gj, slower charging time from upstream cells conspires with acceler
279  track phase transformation as a function of charging time in individual lithium iron phosphate batte
280 mal low emission charging scenario, matching charging time with the lowest available MEF.
281 a discrete-time feedback loop that equalizes charging time, digitize temperature directly.
282         A feedback-control protocol based on charging-time compensation was introduced.
283                                    The short charging times and high power capabilities associated wi
284            Supercapacitor fibers, with short charging times, long cycle lifespans, and high power den
285  by lack of charging infrastructure and long charging times.
286 odel that defines conditions for exponential charging to occur and provides insights into the mechani
287 photogenerated holes from the semiconductor, charging to potentials sufficient to drive water oxidati
288                  Importantly, the time for a charging transient to reach equilibrium was found to be
289  that do not directly depend on potential or charging transients.
290 (ARSs) are essential enzymes responsible for charging tRNA molecules with cognate amino acids.
291 ons factors associated with electric-vehicle charging using 10 methods at nine charging station locat
292  as they undergo progressive electrochemical charging via ion (de)insertion.
293  cathode, for example, from ~1 to 1.84 for a charging voltage of 0.4 V.
294 lculated specific charge generated by corona charging was in good agreement with the experimental res
295 he twisting of the double helicene core upon charging was observed.
296 e apparent lack of dendrite formation during charging which is one of the crucial concerns of using a
297  increased upper cutoff voltage (UCV) during charging, which delivers significantly increased specifi
298                                  We simulate charging with a discrete-element model including electri
299                                The increased charging with the smaller tip sizes for proteins with a
300 no acid starvation or interference with tRNA charging without affecting the endoplasmic reticulum unf

 
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